The Carnot cycle is a thermodynamic cycle that can be invented by French Physicist Sadi Carnot in 1824.
In the Carnot cycle, two reversible isothermal processes and two reversible adiabatic processes are done in a heat engine.
The Carnot cycle consist of four processes following below :
Q1 = Heat addition = R T1 ln v2
/ v1
What is the Carnot cycle?
In the Carnot cycle, two reversible isothermal processes and two reversible adiabatic processes are done in a heat engine.
Process of Carnot cycle :
The Carnot cycle consist of four processes following below :
- A reversible isothermal gas expansion process. From the diagram shown below the ideal gas in the system absorbs some amount of heat from the heat source at a high temperature and then expands thus the work was done on surroundings.
- A reversible adiabatic gas expansion process. In this process, the system is thermally insulated. The gas expands continuously and does work on surrounding, which causes the system to cool to a lower temperature.
- A reversible isothermal gas compression process. In this process, work has done surrounding gas and cause a loss of heat.
- A reversible adiabatic gas compression process. In this process, surrounding continue to do work to a gas, which causes the temperature to rise back to high temperature attain in the first process.
The efficiency of the Carnot cycle :
It can be defined as the ratio of the energy output to the energy input. Here energy output is work done and energy input is heat addition.
From the calculation,
Wnet = R ln v2 / v1 (T1
– T2 )
Ŋcycle = Wnet / Q1 = T1
– T2 / T1
The large back work is a big drawback of this cycle.
Assumption of the Carnot cycle :
- No friction at all between the piston and cylinder and also other moving parts of the engine, thus there is no heat generated and lost due to friction.
- There is no transfer of heat with the external atmosphere because the engine is completely insulated.
- There is also no exchange of heat between various parts of the engine.